Parallel imaging based on expanded unfolding technique

ABSTRACT

Parallel imaging is performed by a magnetic resonance imaging system provided with a multiple RF coil composed of plural element coils. As part of parallel imaging conditions, a desired imaging FOV and a reduction rate of data acquisition time for parallel imaging are specified by an operator. An unfolding FOV to which an unfolding scale is assigned is specified. The unfolding scale is larger in value than the reduction rate, thus the unfolding FOV is larger in size than the imaging FOV. Using an acquisition FOV specified based on the imaging FOV and the reduction rate, a scan for parallel imaging is performed and images are reconstructed corresponding to the respective element coils. The reconstructed images are unfolded into an unfolding-FOV image at the unfolding scale. An image having the imaging FOV is cut out, as a desired final image, from the unfolded image.

BACKGROUND OF THE INVENTION

1. Technical Field of the Invention

The present invention relates to a magnetic resonance imaging (MRI)apparatus capable of performing parallel imaging (PI). In particular,the present invention relates to both magnetic resonance imaging systemsand parallel imaging methods which reduce artifacts inherent to parallelimaging by improving a post-processing unfolding technique.

2. Related Art

Magnetic resonance imaging constructs images from MR signals emanatedfrom an object in response to magnetically excited nuclear spins of theobject in a static magnetic field at a Larmor frequency of the spin.

In the field of magnetic resonance imaging, study of fast imaging hasbecome active. For example, a fast imaging technique called in generalparallel imaging has been known, which requires a multiple RF coilconsisting of a plurality of RF coils (i.e., element coils). Thisparallel imaging technique has historically been called “multicoil fastimaging technique,” “PPA (Partially Parallel Acquisition) technique,”and/or “subencoding technique.”

Parallel imaging can be performed in a variety of modes, which include(1) a technique of calculating data to be skipped in k-space; (2) atechnique of unfolding data in real space (called a “subencodingtechnique” or a “SENSE technique”), and (3) a technique of combiningSum-Of-Square images (called a “PILS”-technique) formed from thesubencoding or SENSE technique. Techniques belonging to mode (2) havebeen known by such references as “Ra J. B. and Rim C. Y., Fast ImagingMethod Using Multiple Receiver Coils with Subencoding Data Sets, ISMRMp.1240, 10991”; “Ra J. B. and Rim C. Y., Fast Imaging Using SubencodingData Sets From Multiple Detectors, MRM 30:142-145, 1993”; “Pruessman K.P., Weiger M., Scheidegger M. B., and Boesiger P., SENSE: SensitivityEncoding for Fast MRI, MRM 42:952-962, 1999”; and “Japanese patentpublication No. WO99/54746(1998)”.

Basically, these techniques for parallel imaging uses an array coil(hereinafter referred to as Phased Array Coil: PAC) composed of aplurality of RF coils (i.e., element coils), which is one kind of amultiple RF coil, and adopts subencoding acquisition. This subencodingacquisition requires that phase encoding be skipped every so manypredetermined steps, so that the total number of phase encoding steps isreduced down to an amount equal to “1/the number of RF coils” from thepredetermined number of phase encoding steps otherwise necessary forreconstructing an ordinary image (i.e., with no skipped phase encodingsteps).

The respective RF coils receive echo signals in a concurrent manner. Theecho signals received by each RF coil are used to produce a set of imagedata. Hence FOV (field of view) of each image, which is produced fromecho signals acquired by each RF coil having a smaller individual FOV,whereby scan time is shortened for fast imaging.

However, such an image produced using echo signals acquired by each RFcoil includes wrap-around or folding (which is also called “aliasing”)in edge regions of each image. In parallel imaging, the fact that pluralRF coils have different sensitivity distributions is thus utilized toperform, as post-processing, unfolding to unfold each image acquiredusing each RF coil. This unfolding is processed based on the spatialsensitivity maps of the RF coils.

A plurality of pieces of images, which have been subjected to unfoldingprocessing, are then combined into a final full-FOV image. Therefore,the parallel imaging technique is able to accelerate to a fast scan(i.e., fast imaging) and finally provide wide FOV-images covering, forexample, the whole abdominal area of an object to be scanned.

However, as described above, in the case of the parallel imaging, it istheoretically inevitable that each image acquired using each RF coil issubjected to the folding phenomenon. There is a problem in that thereremain artifacts due to the folding, which are known as back-folding, aslong as the existence region of an object to be scanned is within FOVspecified as one imaging parameter.

To be specific, conventional parallel imaging plans a scan, in whichconditions of unfolding processing are decided according to a finalimage specified by an operator with the use of such parameters as ROI,matrix size, FOV given during an imaging plan. The final image isnormally rectangular in the shape. The decided unfolding processingconditions are used to produce unfolded images. In order to perform theunfolding processing in a preferable manner, operators should specifythe size of a ROI (region of interest) exactly including the existenceregion of each object to be scanned. However, in practical clinicalexaminations, exactly specifying such ROIs becomes a considerable burdenon operators. It is thus easier for operators to roughly specify theROIs, resulting in back-folding artifacts occasionally occuring anddeteriorating image quality for interpretation.

With reference to FIGS. 1A to 1C, such conditions will now be detailed.

FIG. 1A illustrates one conventional example in which a ROI defining aregion subjected to an MR scan is set in a proper manner. A ROI is givenso as to completely cover an object to be scanned and imaging conditionsare given through a scan plan, before the subencoding technique isapplied to data acquisition from the object. In this example, thesubencoding technique is performed with the number of phase encodingsteps reduced to one half of that required for standard Fourier imaging,so that the reduction rate of data acquisition time is 2 (i.e., two-foldspeed). The folding, in this example, will cause superposition at twopositions between adjacent folded FOVs. Hence, applying the unfoldingprocessing on the assumption that two positions between adjacent foldedFOVs are merely superposed with each other provides an image with nofolded FOVs.

On the other hand, FIG. 1B illustrates another conventional example inwhich a ROI for imaging is set improperly. To be specific, during a scanplan for setting various imaging parameters, the ROI has been placed tospecify an FOV (corresponding to the size of a desired final image)smaller than the actual existence region of an object to be scanned. Inthis example, when performing a scan at the foregoing two-fold speed,the folding will cause, in part, superposition between two folded FOVs,that is, superposition of three positions belonging to the three FOVs.This folding cannot be removed even if the unfolding processing on theforegoing two-fold speed is executed.

FIG. 1C exemplifies a conventional plan carried out in the manner shownin FIG. 1B, but subjected to imaging other than parallel imaging.However, in the example shown in FIG. 1C, since folding is caused onlyat edges of the FOV, there occurs no serious diagnostic problem inobserving the final image.

When making reference to only FIGS. 1A to 1C, it may seem that theforegoing problem can easily be removed by merely setting, during a scanplan, a rectangular FOV slightly larger than a final-image desired size.In practice, however, the elimination of the problem will not be sosimple. A multi-slice imaging technique is frequently adopted in theactual clinical application, where a ROI on one or more slices otherthan a slice used for a scan plan may be set to be less than theexistence region of an object. Namely the existence region is beyond theFOV given through the ROI that has been set, like FIG. 1B. Hence thecurrent situation is that it is not easy to always set a proper ROI.FIG. 2 illustrates such an undesirable situation, in which one of theslices suffers from the fact that a ROI is given improperly.

In imaging the heart, scans are normally made along the minor axis,major axis, and/or sections in the four chambers. FIGS. 3A and 3Bpictorially illustrate some types of imaging of the heart along theminor axes thereof. However, this imaging also frequently suffers theforegoing problem, because the sectional shapes themselves of the heartare complicated and sections differ largely patient by patient. Inaddition, the same problem may occur in imaging a baby in the womb,because it is required that a section to be scanned coincide with thebaby's orientation.

Even for imaging a coronal image of the trunk, it appears to be areality that it is difficult to plan a proper FOV completely including adesired trunk section, because the arms positioned by the trunk extendlargely in the lateral direction.

As understood from the above, a proper scan plan for the parallelimaging technique is not always carried out.

SUMMARY OF THE INVENTION

The present invention has been made with due consideration to theforegoing difficulties, and an object of the present invention is toprovide a magnetic resonance imaging system and a method for parallelimaging that (i) provides stable and reliable reconstructed images(leading to a high-quality final image) with unfolding artifacts removedor suppressed steadily, regardless of how an FOV specified as an imagingregion during a scan plan is positionally related to an object'sexistence region and (ii) alleviates operator's labor and time necessaryfor specifying the FOV (broadly, the scan plan) so that patientthroughput is improved.

In order to accomplish the above object, the magnetic resonance imagingsystem and the method for parallel imaging responds to an FOV (i.e.,imaging FOV or planned FOV) specified as an imaging region by anoperator during a scan plan, the response being outlined as follows. Anintervening virtual FOV for unfolding (called “unfolding FOV”), the sizeof which is larger than that of the FOV specified during the scan plan,is automatically specified by the magnetic resonance imaging system. Inthe system, this unfolding FOV is subjected to unfolding, into anintervening image, reconstructed images acquired by parallel imaging. Afinal image having the operator-specified FOV (i.e., imaging FOV orplanned FOV) or a further FOV relating to the operator-specified FOV iscut out from the intervening image on the unfolding FOV. Hence a desiredfinal image on the parallel imaging can be obtained using theintervening FOV.

Practically, the present invention provides, as one aspect, a magneticresonance imaging system provided with a multiple RF coil composed of aplurality of element coils and configured to use the multiple RF coil toperform parallel imaging with an object to be imaged. The systemcomprises an imaging FOV specifying unit specifying a desired imagingFOV (Field Of View); an acquisition FOV specifying unit specifying anacquisition FOV on a basis of the imaging FOV, the acquisition FOV beingused in performing a scan for parallel imaging; an unfolding FOVspecifying unit specifying an unfolding FOV larger in size than theimaging FOV; an image acquisition unit configured to perform the scanwith the object on a basis of the acquisition FOV so that areconstructed image having the acquisition FOV is acquired for everyelement coil in response to the scan; an unfolding processing unitconfigured to apply, on a basis of the unfolding FOV, unfoldingprocessing to the acquisition-FOV reconstructed image acquired by theimage acquisition unit so that the acquisition-FOV reconstructed imageis unfolded to provide an image having the unfolding FOV; and an imageproducing unit producing an image having the imaging FOV from theunfolding-FOV image obtained by the unfolding processing unit.

In this configuration, it is preferred that the imaging FOV specifyingunit includes a unit for specifying imaging conditions for parallelimaging including both the imaging FOV and a reduction rate of dataacquisition time for parallel imaging, the acquisition FOV specifyingunit is configured to specify an acquisition FOV directed to the scanfor parallel imaging depending on the reduction rate, the unfolding FOVspecifying unit being configured to specify an unfolding scale (i.e., arate for unfolding reconstructed images that are wrapped around)assigned to the unfolding FOV, the unfolding scale being larger innumerical value than the reduction rate, and the image producing unitbeing configured to produce the imaging-FOV image by cutting out theimaging-FOV image from the unfolding-FOV image obtained by the unfoldingprocessing unit.

Preferably, the unfolding scale assigned to the unfolding FOV is aninteger larger in a numerical value than the reduction rate specified aspart of the imaging conditions. Hence the unfolding FOV is expanded morethan the imaging FOV.

The present invention provides, as another aspect, a magnetic resonanceimaging system provided with a multiple RF coil composed of a pluralityof element coils and configured to use the multiple RF coil to performparallel imaging with an object to be imaged. The system comprises animaging condition specifying unit specifying imaging conditionsincluding an imaging FOV for parallel imaging and a reduction rate ofdata acquisition time for parallel imaging; a scan unit performing ascan for parallel imaging to acquire echo signal from the element coils;a reconstruction unit reconstructing, into images, the echo signalsdetected by the element coils; an unfolding unit unfolding thereconstructed images into an unfolded image at an unfolding scale lagerthan the reduction rate; and an image cutting-out unit cutting out animage having the specified imaging FOV from the unfolded image.

In this case, it is preferred that the unfolding scale is an integerlarger than the reduction rate, thus providing an unfolding FOV that isexpanded more than the imaging FOV.

Further, the present invention provides, as another aspect, a method ofperforming parallel imaging by a magnetic resonance imaging systemprovided with a multiple RF coil composed of a plurality of elementcoils and configured to use the multiple RF coil to perform parallelimaging with an object to be imaged, comprising: specifying a desiredimaging FOV (Field Of View); specifying an acquisition FOV on a basis ofthe imaging FOV, the acquisition FOV being used in performing a scan forparallel imaging; specifying an unfolding FOV larger in size than theimaging FOV; performing the scan with the object on a basis of theacquisition FOV so that a reconstructed image having the acquisition FOVis acquired for every element coil in response to the scan; applying, ona basis of the unfolding FOV, unfolding processing to theacquisition-FOV reconstructed image so that the acquisition-FOVreconstructed image is unfolded to provide an image having the unfoldingFOV; and producing an image having the imaging FOV from theunfolding-FOV image.

In this way, for performing the unfolding processing in parallelimaging, the present exemplary embodiments adopt the “expanded unfoldingtechnique” (so-termed by the present inventors),” which is a techniqueof virtually expanding a region to be unfolded. Hence, however anoperator specifies a region to be imaged in a scan plan, the unfoldingprocessing can be carried out to provide an optimum result at any time.It is therefore possible to reduce, to a great extent, without fail,artifacts due to the unfolding phenomenon inherent to parallel imaging.An operational burden on operators can also be alleviated, which willlead to a stable supply of high-quality images, thereby enhancing theusefulness of parallel imaging.

BRIEF DESCRIPTION OF THE DRAWINGS

In the accompanying drawings:

FIGS. 1A to 1C explain conventional unfolding techniques for parallelimaging, respectively;

FIG. 2 explains a drawback with respect to conventional unfoldingtechniques for parallel imaging;

FIGS. 3A and 3B are other illustrations for explaining a drawback withrespect to conventional unfolding techniques for parallel imaging;

FIG. 4 is a functional block diagram exemplifying the configuration of amagnetic resonance imaging system according to an example of the presentinvention;

FIG. 5 is a flowchart outlining parallel imaging carried out in thefirst embodiment;

FIG. 6 explains a relationship between a set of FOVs (Field Of Views) (,which represent changes from an FOV specified in a scan plan to an FOVfinally imaged) and sectional regions of an object to be scanned, theFOVs being directed to an expanded unfolding technique according to thefirst embodiment;

FIG. 7 explains an example of a relationship between a set of FOVs (,which represent changes from an FOV specified in a scan plan to an FOVfinally imaged) and sectional regions of the heart of an object to bescanned, the sectional regions being along the minor axis of the heartand the FOVs being directed to the expanded unfolding techniqueaccording to the first embodiment;

FIG. 8 explains another example of a relationship between a set of FOVs(, which represent changes from an FOV specified in a scan plan to anFOV finally imaged) and sectional regions of the heart of an object tobe scanned, the sectional regions being along the minor axis of theheart and the FOVs being directed to the expanded unfolding techniqueaccording to the first embodiment;

FIG. 9 explains an example of a relationship between a set of FOVs (,which represent changes from an FOV specified for data acquisition to anFOV finally imaged) and sectional regions of an object to be scanned,the FOVs being directed to an expanded unfolding technique according toa second embodiment, the expanded unfolding technique involving controlof an unfolding scale based on a mask;

FIG. 10 is a flowchart outlining parallel imaging carried out in thesecond embodiment;

FIG. 11 explains another example of a relationship between a set of FOVs(, which represent changes from an FOV specified for data acquisition toan FOV finally imaged) and sectional regions of an object to be scanned,the FOVs being directed to an expanded unfolding technique according tothe second embodiment, the expanded unfolding technique involvingcontrol of an unfolding scale based on a mask; and

FIG. 12 explains an expanded unfolding technique carried out in a thirdembodiment of the present invention, using a glued unfolding techniquebased on a trapezoidal mask.

DETAILED DESCRIPTION OF PREFERRED EMBODIMENTS

With reference to accompanying drawings, a magnetic resonance imaging(MRI) apparatus according to various embodiments of the presentinvention will now be described.

First Embodiment

Referring to FIGS. 4 to 8, a magnetic resonance imaging system accordingto a first embodiment of the present invention will now be described. Inthe present embodiment, this magnetic resonance imaging system will beexplained as a system capable of performing parallel imaging.

At first, referring to FIG. 4, the overall configuration of a magneticresonance imaging system according to the present embodiment will now beoutlined.

The magnetic resonance imaging system is provided with a multiple RFcoil and performs parallel imaging using the multiple RF coil to produceMR images. As shown in FIG. 4, this system is also provided with a couchblock, a static magnetic field generating block for generating a staticmagnetic field, and a gradient generating block for adding positioninformation to the static magnetic field. The system is also providedwith a transmission/reception block for transmitting and receiving RFsignals and a control/calculation block that is in charge of control ofthe overall system and image reconstruction.

Of these components, the static magnetic field generating block isprovided with a magnet 1 constructed by employing for example asuperconducting magnet and a static power supply 2 supplying current tothe magnet 1. By these devices, a static magnetic field Ho is producedin an axial direction of a cylindrical bore (a space for diagnosis) intowhich an object P to be imaged is inserted. In the orthogonal coordinateaxes assigned to the system, the axial direction agrees with the Z-axisdirection. In addition, this generation block is also provided with anot-shown shimming coil to which current is supplied from a shimmingcoil power supply to shim the static magnetic field.

The couch block is configured to have a not-shown patient couch and atabletop 14T that is able to slidably travel along the upper surface ofthe patient couch and to be driven by a couch drive unit 14D. The objectP is laid on the tabletop 14T and can be inserted and returned into andfrom the bore of the magnet 1. The couch drive unit 14D performs thisinsertion and return. That is, the couch drive unit 14D responds to adrive signal given by a host computer 6 later described so as to movethe tabletop 14T along its longitudinal direction (i.e., the Z-axisdirection). The object P is laid on the tabletop 14T along itslongitudinal direction, for example.

The gradient generating block has a gradient coil unit 4G incorporatedin the magnet 1. The gradient coil unit 4G includes not-shown three sets(types) of x-, y-, and z-coil for generating gradient magnetic fields(gradients) in the X-, Y-, and Z-axes directions that are orthogonal oneanother. This gradient generating block is further provided with agradient amplifier 4 to supply currents to each of the x-, y-, andz-coils. The gradient amplifier 4 supplies those coils with pulsedcurrents to generate gradients under the control of a sequencer 5 laterdescribed.

Controlling pulsed currents supplied from the gradient amplifier 4 tothe x-, y-, and z-coils enables the mutually-orthogonal X-, Y-, andZ-directional gradients, which are gradients in the physical axes, to besynthesized. Thus mutually-orthogonal logic directional gradients, i.e.,a slice gradient Gs, phase-encode gradient Ge, and read-out (frequencyencoding) gradient Gr can be set or changed in an arbitrary manner. Thegradients in the slice, phase-encode, and read-out directions aresuperposed on the static field Ho.

The transmission/reception block is provided with a whole-body (WB) coil7T and receiving multiple RF coils 7R, both of which are formed as RFcoils, and a transmitter 8T and a receiver 8R both connected to thecoils 7T and 7R. The coils 7T and 7R are disposed in the vicinity of theobject P placed in the space for diagnosis formed within the bore of themagnet 1.

The whole-body coil 7T is used in common for transmission and receptionof RF signals in cases where the coil 7T is employed as the sole RFcoil. By contrast, when employing the multiple RF coils 7R (serving as areception coil), the whole-body coil 7T is used as a RF coil dedicatedto transmission of RF signals.

The multiple RF coil 7R, which is formed as a whole as an array type ofcoil of which S/N (signal-to-noise ratio) can be set higher, is composedof a plurality of RF coils 7 a, 7 b, 7 c and 7 d each of which is anelement coil. In the present embodiment, the four RF coils 7 a, 7 b, 7 cand 7 d (that is, four detecting channels) are adopted and each of theRF coils 7 a to 7 d is formed as a surface coil shaped, for example,into a circle or rectangle. The sizes and shapes of the RF coils 7 a to7 d are decided such that those four-channel RF coils are able to covera desired FOV (corresponding to a region of interest).

The output signals from those four-channel RF coils 7 a to 7 d aresupplied to a receiver 8R (composing part of the transmission/receptionblock) independently of each other.

The coil configuration shown in FIG. 4 pictorially illustrates thefour-channel RF coils 7 a to 7 d arranged along the body surface of theobject P. However, the multiple RF coil 7R is not always limited to acoil configuration composed of plural surface coils, as described above,but may be composed of plural volume coils or of a QD (Quadrature) coil.As another modification, the multiple RF coil may be attached to thecouch or object.

The transmission/reception block will now be described. This block isprovided with a transmitter 8T and the receiver 8R, which are operativeunder the control of a sequencer 5 later described.

The transmitter 8T supplies to the whole-body coil 7T RF pulsed currentsof which frequency is set to a Larmor frequency to cause nuclearmagnetic resonance (NMR) at magnetic spins of the object P. In contrast,the receiver 8R receives an echo signal (RF signal) received by thewhole-body coil 7T or multiple RF coil 7R, and then processes it intoecho data (i.e., original data).

Specifically, the receiver 8R is divided, as shown in FIG. 4, into areception part for the whole-body coil and a further reception part forthe multiple RF coils.

The reception part for the whole-body coil includes a duplexer 81connected with the whole-body coil 7T, a preamplifier 82 connected tothe duplexer 81, and a receiving circuit 83 receiving a reception signalfrom the preamplifier 82. The duplexer 81 is coupled with thetransmitter 8T as well.

This connection permits the duplexer 81 to pass a transmission drivepulse from the transmitter 8T to the whole-body coil 7T in transmissiontiming, while to pass an echo signal detected by the whole-body coil 7Tto the preamplifier 82 in reception timing. The preamplifier 82pre-amplifies the received echo signal to send the amplified signal tothe receiving circuit 83. This circuit 83 performs various types ofsignal processing on the inputted echo signal, the processing includingintermediate-frequency conversion, phase detection, low-frequencyamplification, and filtering. In the circuit 83, the processed signal isthen subject to A/D conversion to be produced into echo data (originaldata), before being sent to the host computer 6.

In contrast, the reception part for the multiple RF coils is providedwith four-channel preamplifiers 85A to 85D and four-channel receivingcircuits 86A to 86D, which are connected serially in every receptionchannel. The output terminals of all the receiving circuits 86A to 86Dare electrically connected to the host computer 6. Hence in thereception part for the multiple RF coils, four-channel echo signalsdetected by the four-channel RF coils 7 a to 7 d are routed to thereceiving circuits 86A to 86D via the amplifiers 85A to 85D,respectively. Like the foregoing, in each of the receiving circuit 86Ato 86D, the inputted echo signal is subjected to various types ofprocessing, such as intermediate-frequency conversion, phase detection,low-frequency amplification, and filtering. Further, in each receivingcircuit 86A (to 86D), the processed echo signal further undergoes A/Dconversion to be produced into echo data. The thus-processed echo datais then sent from each of the receiving circuits 86A to 86D to the hostcomputer 6.

The control/calculation block will now be explained, which includes asequencer 5 (also called sequence controller), host computer 6, storage11, display 12, and input device 13.

Of these components, the host computer 6 operates based on softwareprocedures memorized in its inner memory and/or the storage 11. Theoperations of the host computer 6 include various types of preparationscans for parallel imaging, a scan plan, an imaging scan, and a set ofprocedures for post-processing. The preparation scans include a pilotscan for positioning, a shimming scan for informing the static magneticfield, and a sensitivity-map scan for measuring a sensitivity map ofeach element coil (i.e., each RF coil 7 a (to 7 d)) used for unfolding.When the preparation scans and the imaging scan are performed, the hostcomputer 6 provides the sequencer 5 with pulse sequence informationnecessary for those scans.

Moreover, the host computer 6 performs a variety of types of processing.One type of processing is a man-to-machine interface. During a scanplan, the host computer 6 is able to function, in conjunction with boththe display 12 and input device 13, as an interface between an operatorand the system. This interface function allows the operator toinformation about the scan plan to the system in an interactive manner.The scan plan includes the specification of imaging conditions(parameters), such as the phase-encode direction and the position, sizeand shape of a desired FOV in parallel MR imaging.

Other types of processing are computing functions, which include theestimation of a sensitivity map of each of the RF coils 7 a to 7 d thatcompose the multiple RF coil 7R, the calculation of image data byapplying reconstruction processing to the acquired echo data, and thecontrol of drive of the couch drive unit 14D.

The pulse sequence information is specified to make a scan produce oneor more sets of echo data necessary for reconstructing one or moreimages, once the scan is carried out on the pulse sequence information.The pulse sequence is a sequence on either a three-dimensional (3D) scanor a two-dimensional (2D) scan. As practical modes of pulse trains whichcan be employed, provided are an SE (spin echo) method, FSE (fast spinecho) method, FASE (fast asymmetric SE) method (that is, the FSE methodcombined with a half-Fourier method), EPI (echo planar imaging) method,FE (gradient field echo) method, FFE (fast FE) method, segmented FFEmethod, and others.

The sequencer 5 has a CPU and memories and memorizes pulse sequenceinformation sent from the host computer 6. Based on this information,the sequencer 5 controls the operations of the gradient amplifier 4,transmitter 8T, and receiver 8R. The pulse sequence information is allkinds of information necessary for operating the gradient amplifier 4,transmitter 8T, and receiver 8R according to a series of pulse sequencesthat is specified. For instance, the pulse sequence information includespieces of information concerning magnitudes of pulsed currents appliedto the x-, y-, and z-coil, durations of application of the pulses, andapplication timing.

Data of images reconstructed and combined in parallel imaging aredisplayed on the display 12 and stored in the storage 11. The inputdevice 13 is used for sending, to the host computer 6, information inrelation to imaging conditions (parameters), pulse sequence, combinationof images, and subtraction between images.

How to specify FOVs for the unfolding processing executed in theparallel imaging according to the present embodiment will now beexplained in terms of its theory (refer to FIG. 6, for example).

Unlike the conventional, this unfolding processing is based on thetechnique of specifying a “planned FOV” in planning a scan, acquiringecho signals based on an “acquisition FOV” of which region is narrowerthan that of the “planned FOV,” automatically specifying an “unfoldingFOV” serving as an “intervening FOV” and having a region larger than aregion of the “planned FOV,” using this “unfolding FOV” to process imagedata into an image, and cutting out an image of a desired “final FOV”from the image of the “unfolding FOV.” The “unfolding FOV” is specifiedindependently of the “planned FOV.” By way of example, the “final FOV”is equal in the size to the “planned FOV.”

The relationship among those FOVs is as follows.

<Planned FOV> The “planned FOV,” which is denoted as L_final, is an FOVrepresenting a desired imaging region specified by an operation inplanning a scan for setting various imaging conditions (parameters).When the scan plan is conducted, a reduction rate R for data acquisition(that is, a scale for parallel imaging) is specified jointly.

<Acquisition FOV> The “acquisition FOV,” which is denoted as L_acquis,is an FOV to be used for acquiring echo signals from each element coiland defined as L_acquis=L_final/R.

<Unfolding FOV> The “unfolding FOV (i.e., intervening FOV)” is denotedas L_unfold defined by L_unfold>L_final=R·L_acquis.

<Final FOV> The “final FOV,” for example, corresponds to the “plannedFOV” and an image of this final FOV is obtained by cutting out an imageproduced using the unfolding FOV. In this way, it is normal that theplanned FOV is equal in the size to the final FOV (i.e., an FOV to besubjected to final imaging), but this is not a definitive list. Ifneeded, it may be possible to specify a planned FOV not equal in thesize to a final FOV (the planned FOV≠the final FOV).

Compared to how to use the above-listed FOVs, it can be said that theconventional use of FOVs in the unfolding processing is based on arestriction of “planned FOV”=“folding FOV”=“final FOV.”

The present invention removes such a restriction and adopts a way ofsetting a relation that the “unfolding FOV” is larger in the size thanthe “final FOV (for example, “planned FOV)” (the “unfolding FOV”>the“final FOV”). This improves the conventional drawback and provides agreat advantage to practical use, as will be described below.

In the present invention, a region subjected to the unfolding necessaryfor parallel imaging is expanded in an imaginary manner, so that theinventors term this way as an “Expanded Unfolding Technique.”

Hence an unfolding scale R′ on the “expanded unfolding technique” can beexpressed as bellow. $\begin{matrix}{R^{\prime} = {{{L\_ unfold}/{L\_ aquis}} > {{L\_ final}/{L\_ aquis}}}} \\{= {\left( {R \cdot {L\_ acquis}} \right)/{L\_ aquis}}} \\{= R}\end{matrix}$

That is, the unfolding scale R′ is set to meet the numericalrelationship of R′>R. Preferably, the unfolding scale R′ is set to anyinteger to satisfy the relationship of R′>R. A practical example of theunfolding scale R′ is Int(R)+1 (Int: integer part). For example, whenR=2 is specified, the unfolding scale R′ is set to any one of 3, 4, . .. , etc. When R=1.5 is specified, the unfolding scale R′ is set to anyone of 2, 3, . . . , etc. When R=3 is specified, the unfolding scale R′is set to any of 4, 5, 6, . . . , etc. Alternatively, the unfoldingscale R′ may be set to R′=Nc, in which Nc is the number of receptionchannels which is an upper limit of the unfolding scale R′.

However, when the scaling factor R′ is too large, a “g” factor becomeslarge as well, resulting in a lowered SNR. In addition, the unfoldingrequires a sensitivity map of each element coil. Hence the unfoldingscale R′ should be a value less than a range in which there existsensitivity maps for simply unfolding in all regions. By the way, the“g” factor is an indication showing a decrease in the SNR, which is dueto the unfolding (refer to “Pruessman K, et at., SENSE: SensitivityEncoding for Fast MRI, MRM 42:952-962, 1999”)

Referring to FIGS. 5 to 8, the overall operation of parallel imaging onthe “expanded unfolding technique” will now be exemplified.

When parallel imaging is commanded, the host computer 6 executes theprocessing in the procedures shown in FIG. 5.

First of all, the host computer 6 registers a patient using informationcoming from an operator (step S1). The host computer 6 then participatesin a pilot scan for positioning, which is carried out using thewhole-body coil 7T, whereby a positioning image is acquired (step S2).In cases where such a positioning image has already been acquired, thealready-acquired positioning image can be used instead, thus omittingthe pilot scan.

The host computer 6 executes the shimming scan (step S3), and thenexecutes a sensitivity-map scan for acquiring sensitivity map data ofthe RF coils 7 a to 7 d serving as element coils (step S4). It is notalways true that this sensitivity-map scan precedes the imaging scanlater described. The sensitivity-map scan may be performed as part of aseries of pulse trains prepared for the imaging scan.

After the above preparation scans are completed, the host computer 6moves its operation to a scan plan (setting of the imaging conditions)(step S5A). During the scan plan, the host computer 6 behaves as aninterface with an operator who observes the positioning image tointeractively give necessary information.

Practically, at step S5A, the host computer 6 receives information inrelation to both of a reduction rate for parallel imaging (i.e., a scalefor parallel imaging) and an FOV (field of view) specified by a ROI(region of interest) showing a desired imaging region (i.e., a plannedFOV), in addition to information indicative of ordinary imagingparameters such as the type of a desired pulse sequence.

At step S5B, the microcomputer 6 makes a response to this reception suchthat the host computer 6 automatically computes an acquisition FOV andmemorizes data of the computed acquisition FOV. At steps S5C and S5D,the host computer 6 reads out an appropriately predetermined unfoldingscale R′, and then uses the read-out unfolding scale R′ to automaticallycompute data of an unfolding FOV. The data of the unfolding FOV ismemorized.

After this, the host computer 6 makes the sequencer 5 perform a desiredmode of parallel imaging as the imaging scan under the decidedacquisition FOV (step S6). This imaging enables the microcomputer 6 toreceive echo signals detected by the respective RF coils 7 a to 7 d andto reconstruct the echo signals into images in the actual space (stepS7).

The microcomputer 6 applies unfolding possessing to each of thereconstructed images produced from the echo signals detected by the RFcoils 7 a to 7 d, and then cuts out an image of a desired final FOV fromeach of the unfolded images (steps S8 and S9).

In connection with FIG. 6, the processing for the above unfolding andcutting will now be exemplified. FIG. 6 exemplifies a reduction rate(scale) R of 2 (i.e., two-fold speed) for parallel imaging. Under thesituation where a planned FOV indicating a desired region to be imagedis specified on a positioning image (in this case, the planned FOVsmaller than the existence region of an object is specified), parallelimaging is performed at the reduction rate R of 2 (in other words,subencoding data acquisition at the two-fold speed). Hence, using eachof the RF coils 7 a to 7 d, data to be mapped in an acquisition FOVcorresponding to ½ of the overall matrix is acquired (refer to FIGS.6(a) and (b)).

In this example of the present embodiment, in the magnetic resonanceimaging system, an unfolding scale R′ larger than the reduction rate Ris specified automatically (with the operator unconscious of thisautomatic setting of the reduction rate R). For example, the unfoldingscale R′ is specified as three-fold speed (i.e., R′=3), and unfoldingprocessing is applied to the unfolding FOV corresponding to R′=3, byusing the sensitivity map data of each of the RF coils 7 a to 7 d (referto FIG. 6(c)). In the imaging carried out in an ordinary fashion, theunfolding FOV corresponding to the unfolding scale R′=3 can contain,without fail, the existence region of an object to be imaged.Accordingly, the host computer 6 cuts out, from a real-space image ofthe unfolding FOV, an image of which size equals the desired plannedFOV, whereby an image of which size equals a final FOV (i.e., in thiscase, the planned FOV) is produced (refer to FIG. 6(d)). Thiscutting-out processing is also executed automatically in the magneticresonance imaging system (it is not required that the operator beconscious of the fact that the cutting-out processing is executed in thesystem).

A real-space image of the final FOV, which has been produced as above,is displayed on the display 12 and stored as image data into the storage11 (step S10 in FIG. 5). This enables the operator to steadily observethe image of which size exactly corresponds to an FOV specified in thescan plan, with the operator unconscious of performing the expandedunfolding technique.

Referring to FIGS. 7 and 8, some applications will now be explained, inwhich the foregoing expanded unfolding technique is applied to sectionsof the heart along its minor axis. In any case, assumptions are madesuch that a reduction rate R of 2 and an unfolding scale R′ of 3 arespecified and an initial minor-axial section of the heart is partiallyprotruded from an FOV specified in planning a scan. In particular,compared to that in FIG. 7, the section in FIG. 8 shows that a plannedFOV is too small to avoid the object from protruding partially but to alarge degree, from the boundary of the planned FOV. Employing theexpanded unfolding technique, however, makes it possible to produce adesired final-FOV image in either case.

In this way, in the present embodiment, the expanded unfolding techniqueis employed, in which a region applied to the unfolding is made large ina virtual manner. Using this temporarily expanded region, there isproduced an image in which folding artifacts are surely suppressed orprevented from remaining. The produced image is used to obtain afinal-FOV image through the cutting processing.

As a result, even when a region to be imaged (i.e., a planned FOV)specified in a scan plan is incomplete due to the regional relationshipwith the existence of an object or is partially smaller than theexistence region of an object (in other words, the object protrude inpart from the planned FOV), setting the unfolding FOV allows theunfolding possessing to result in an optimum condition. It is thereforepossible to provide higher-quality images with fewer artifacts.

From a different point of view, a region to be imaged (planned FOV)specified during a scan plan may be rough to some extent. Even in such acase, the magnetic resonance imaging system according to the presentembodiment will automatically perform the expanded unfolding techniqueas one kind of internal processing (with no formal notification of theperformance to the operator). Hence there is no longer necessary thatthe operator be as nervous as the conventional in specifying a region tobe imaged. The labor and time for the manual specification can be saved,thus remarkably relieving the burden on the specification.

(Second Embodiment)

Referring to FIGS. 9 to 11, a second embodiment of the present inventionwill now be explained. The second embodiment is characteristic ofperforming the foregoing expanded unfolding technique together withcontrolling a scale based on mask information. A magnetic resonanceimaging system according to the second embodiment is identical in itshardware to that used in the first embodiment.

First, control of a scale on mask information will now be explained.Though the expanded unfolding technique has been described in the firstembodiment, the number of positions (i.e., pixels) at each of which thefolding (i.e, aliasing) among the acquisition matrices is actuallysuperposed changes position by position (i.e, pixel by pixel).

Hereinafter, for the sake of a simplified explanation, a set ofpositions satisfying an assumption that an object actually exists willbe referred to as “mask.” An explanation is given on the assumption thatthe shape of an object shown in FIG. 9 is identical to a mask.

In FIG. 9, at a position “A” in an “acquisition FOV,” the folding iscaused in such a manner that three positions A1, A2 and A3 mutuallycorresponding to each other in an “unfolding FOV” are superposed one onanother. It is therefore necessary to perform, in fact, the unfoldingprocessing at an unfolding scale of three-fold speed. As to a position“B,” three positions B1, B2 and B3 are superposed one on another at theposition “B,” but no signal will emanate from the position B1 which isparenthesized. It is therefore possible to remove the position B1 fromthe unfolding calculation, so that, from a practical point of view, itis sufficient to apply the unfolding at an unfolding scale of two-foldspeed to the calculation at the position B1.

Hence, with reference to information indicative of the foregoing maskregion, the number of positions is calculated previously, at each ofwhich the folding is superposed within an object's estimated existenceregion or a given expanded region including the object's estimatedexistence region (i.e., the previous calculation of the number ofequivalent positions).

The expanded unfolding technique is applied to each pixel value of areconstructed acquisition-FOV image at an unfolding scale depending onthe number of equivalent positions at each pixel. For example, if thenumber of equivalent positions at a pixel is 2, the expanded unfoldingat an unfolding scale of two-fold speed is performed, while, on the sameimage, if the number of equivalent positions at another pixel is 3, theexpanded unfolding at an unfolding scale of three-fold speed isperformed. A final FOV is used to produce a desired-size image bycutting an unfolding-FOV image in compliance with the FOV specified inthe scan plan.

To use this mask processing technique in combination with the expandedunfolding technique, the host computer 6 performs parallel imagingaccording to the procedures outlined in FIG. 10. Compared to theforegoing procedures illustrated in FIG. 5, both of a scan plan at stepS5 and the unfolding processing at step S8 are differentiated from thosein FIG. 5. The processing at the remaining steps is similar or identicalto that in FIG. 5.

In the scan plan, the host computer 6 manages the specification ofimaging conditions, specification of an acquisition FOV, reading of anunfolding scale, and specification of an unfolding FOV (steps S5A toS5D). After these steps, the host computer 6 produces data of a maskprecisely covering an object's existence region on a preparation imagereconstructed from echo data acquired through a pilot scan (step S5E).Using both of the mask data and a reduction rate R of data acquisitiontime specified in the scan plan (step S5A), the host computer 6calculates the number of equivalent positions at each of which thefolding is caused (i.e., having the same pixel value) (step S5F). Afterthe processes of an imaging scan and image reconstruction (steps S6 andS7), the expanded unfolding processing is executed, as described, withreference to the above-calculated number of equivalent positions (stepS8).

As a result, as to the position “A” in FIG. 9 to which the threepositions A1, A2 and A3 are actually folded back (for the conventionaltechnique, the position “A” is an improperly unfolded point), thethree-fold unfolding processing is conducted based on the expandedunfolding technique according to the present embodiment. In addition, asto the position “B” in FIG. 9 to which only the two positions B1 and B2are actually folded back, the expanded unfolding technique to be appliedis limited to the two-fold unfolding processing. That is, adeterioration in image quality (i.e., a decrease in SNR), which will beresulted from the meaningless three-fold unfolding, is prevented at theposition “B.”

In this way, through the pixel-basis control of the unfolding scalebased on the mask information, the three-fold unfolding processing givespriority to prevention of the folding and the two-fold unfoldingprocessing prevents the SNR from decreasing due to a swell in the “g”factor. Accordingly, the expanded unfolding has a sharp effectiveness.

Moreover, in a situation shown FIG. 11, this expanded unfoldingtechnique in combination with the mask-based unfolding scale controlalso brings out a remarkable advantage. To be specific, although anobject partially protrudes from both ends of a planned FOV (not shown),the number of actual folded positions at any location on an object isnot more than 2, as understood from two representative locations “C” and“D.” That is, since the two-fold unfolding processing is sufficient forany object's locations, a decrease in the SNR is suppressed and limitedwithin an optimum range, while still providing final images with nofolding.

(Third Embodiment)

Referring to FIG. 12, a third embodiment according to the presentinvention will now be described. This embodiment is characteristic ofavoiding a discontinuity in image quality in performing the expandedunfolding technique together with the unfolding scale control on maskinformation. Incidentally, a magnetic resonance imaging system accordingto the third embodiment has the same hardware configuration identical tothat in the first embodiment.

In the foregoing second embodiment, the expanded unfolding technique hasbeen explained under a condition that the unfolding scale is controlledon the pixel basis. To change the unfolding scale results indiscontinuous changes in the “g” factor, with the result that imageinformation may suffer large discontinuous changes which occur betweenadjacent pixels.

To avoid the discontinuity in the image quality on account of such adiscontinuous change in the unfolding scales (i.e., integers), there isproposed an improved technique termed by the present inventors as a“glued unfolding technique.” This glued unfolding technique adopts theprinciple that, in a boundary portion, two images of which unfoldingscales change are continuously weighted and glued to each other.

In the present embodiment, the glued unfolding technique is reduced intopractice as a “trapezoidal mask technique” that uses a trapezoidal maskin conducting the glued unfolding technique. As shown in FIG. 12, anassumption is made such that a mask that exactly traces the outercontour of an object is denoted as M, a region encircling the mask Mwith an appropriate margin is denoted M′, and a trapezoidal mask isdenoted as T. The trapezoidal mask consists of weighting factors thatrepresent “1” in the region M′ but decreases from “1” along atrapezoidal function outside the region M′ in each phase encodedirection.

The host computer 6 performs additional processing, for example, atsteps S5B and S8 in FIG. 10, in such a manner that the followingprocesses [1] and [2] are sequentially calculated with respect to an“acquisition FOV” and resultant values E(yk) are mapped on an“unfolding-FOV” image.

[1] Positional coordinates yk (k=1, 2, . . . , R′) which correspond toeach other as to the folding are obtained. Assume that R1 denotes thenumber of T values (i.e., weighting factor) each satisfying a relationof T value=1, R2 denotes the number of T values each satisfying arelation of 0<T value≦1, and r=ΣT(yk) (0≦R1≦r≦R2).

[2] As to yk of T(yk)=0, a value satisfying E(yk)=0 is to be obtained.On the assumption that there is yk meeting a condition of T(yk)>0, E(yk)directed to each position T(yk) is computed. [2.1] In the case of0<R1=R2(i.e., a set of positions each satisfying T(yk)=1):

The unfolding is performed at an unfolding scale of R1-fold, resultantunfolded values being E1(yk). As to corresponding yk, the value E(yk) isset to E(yk)=E1(yk).

[2.2] In the case of 0=R1<R2) (i.e., a set of positions each satisfyingT(yk)<1):

The unfolding is performed at an unfolding scale of R2-fold, resultantunfolded values being E2(yk). As to corresponding yk, the value E(yk) iscalculated on E(yk)=T(yk) E2(yk).

[2.3] In the case of 0<R1<R2 (i.e., a set of positions satisfyingT(yk)=1 and T(yk)<1 exist in a mixed manner):

The unfolding is performed at an unfolding scale of R1-fold and at anunfolding scale of R2-fold, resultant unfolded values being E1(yk) andE2(yk), respectively.

As to corresponding yk, the value E(yk) is obtained as follows.When T(yk)=1,E(yk)=((r−R 1)/(R 2−R 1))*E 1(yk)+((R 2−r)/(R 2−R 1))*E 2(yk)When T(yk)<1,E(yk)=T(yk)*E 2(yk).

The above shows the way of linearly changing the weighting factor T, butthis is not a definitive list. An alternative is to change the weightingfactor in a sinusoidal pattern.

The trapezoidal mask is practical, because the functional valuesdefining the mask can contain all data necessary for gluing processingwhich sequentially follows the unfolding processing on the gluedunfolding technique.

The present invention may be embodied in other specific forms withoutdeparting from the spirit or essential characteristics thereof. Thepresent embodiments are therefore to be considered in all respects asillustrative and not restrictive, the scope of the present inventionbeing indicated by the appended claims rather than by the foregoingdescription and all changes which come within the meaning and range ofequivalency of the claims are therefore intended to be embraced therein.

The entire disclosure of Japanese Patent Application Ser. No.2003-130408 filed on May 8, 2003 including the specification, claims,drawings and summary are incorporated herein by reference in itsentirety.

1. A magnetic resonance imaging system provided with a multiple RF coilcomposed of a plurality of element coils and configured to use themultiple RF coil to perform parallel imaging with an object to beimaged, the system comprising: an imaging FOV specifying unit specifyinga desired imaging FOV (Field Of View); an acquisition FOV specifyingunit specifying an acquisition FOV based on the imaging FOV, theacquisition FOV being used in performing a scan for parallel imaging; anunfolding FOV specifying unit specifying an unfolding FOV larger in asize than the imaging FOV; an image acquisition unit configured toperform a parallel imaging scan with the object based on the acquisitionFOV so that a reconstructed image having the acquisition FOV is acquiredfor every element coil in response to the scan; an unfolding processingunit configured to apply, based on the unfolding FOV, unfoldingprocessing to the acquisition-FOV reconstructed image acquired by theimage acquisition unit so that the acquisition-FOV reconstructed imageis unfolded to provide an image having the unfolding FOV; and an imageproducing unit producing an image having the imaging FOV from theunfolding-FOV image obtained by the unfolding processing unit.
 2. Themagnetic resonance imaging system according to claim 1, wherein theimaging FOV specifying unit includes a unit for specifying imagingconditions for parallel imaging including both the imaging FOV and areduction rate of data acquisition time for parallel imaging, theacquisition FOV specifying unit is configured to specify the acquisitionFOV directed to the scan for parallel imaging depending on the reductionrate, the unfolding FOV specifying unit is configured to specify anunfolding scale assigned to the unfolding FOV, the unfolding scale beinglarger in numerical value than the reduction rate, and the imageproducing unit is configured to produce the imaging-FOV image by cuttingout the imaging-FOV image from the unfolding-FOV image obtained by theunfolding processing unit.
 3. The magnetic resonance imaging systemaccording to claim 2, wherein the acquisition FOV specifying unit, theunfolding FOV specifying unit, the unfolding processing unit, and theimage producing unit are automatically activated with internalprocessing implemented within the system.
 4. The magnetic resonanceimaging system according to claim 3, wherein the unfolding scaleassigned to the unfolding FOV is an integer larger in numerical valuethan the reduction rate specified as part of the imaging conditions. 5.The magnetic resonance imaging system according to claim 1, comprisingan image storage/display unit performing either one or both of storageand display of the image of the imaging FOV obtained by the imageproducing unit.
 6. The magnetic resonance imaging system according toclaim 2, comprising an estimating unit estimating an existence region ofthe object in real space, wherein the unfolding processing unit isconfigured to apply, with reference to the existence region of theobject, unfolding processing based on the unfolding scale to each pixelof the acquisition-FOV reconstructed image.
 7. The magnetic resonanceimaging system according to claim 6, wherein the estimating unit isconfigured to estimate the existence region of the object from echosignals acquired by a further scan carried out before or during the scanfor parallel imaging by the image producing unit.
 8. The magneticresonance imaging system according to claim 7, comprising a unitperforming the further scan with a whole-body coil arranged around theobject.
 9. The magnetic resonance imaging system according to claim 6,wherein the unfolding processing unit is configured to obtain the numberof equivalent folded positions in the existence region of the object ora region enlarged to include the existence region, for every pixel onthe reconstructed image obtained by the image producing unit, and toapply the unfolding processing based on the unfolding scale to theacquisition-FOV reconstructed image, the unfolding scale depending onthe number of equivalent folded positions.
 10. The magnetic resonanceimaging system according to claim 6, comprising means for securing acontinuity of pixel values in a pixel-value-discontinuous area on theunfolding-FOV image unfolded by the unfolding processing unit, theunfolding scale being changed discontinuously in thepixel-value-discontinuous area.
 11. The magnetic resonance imagingsystem according to claim 10, wherein the continuity securing means isconfigured to mutually glue different unfolding-FOV images which areunfolded at different scales and subjected to smooth weighting in thepixel-value-discontinuous area.
 12. The magnetic resonance imagingsystem according to claim 11, wherein the continuity securing means usesa trapezoidal mask to give smooth weighting to pixel values in thepixel-value-discontinuous area.
 13. A magnetic resonance imaging systemprovided with a multiple RF coil composed of a plurality of elementcoils and configured to use the multiple RF coil to perform parallelimaging with an object to be imaged, the system comprising: an imagingcondition specifying unit specifying imaging conditions including animaging FOV for parallel imaging and a reduction rate of dataacquisition time for parallel imaging; a scan unit performing a scan forparallel imaging to acquire echo signals from the element coils; areconstruction unit reconstructing, into images, the echo signalsdetected by the element coils; an unfolding unit unfolding thereconstructed images into an unfolded image at an unfolding scale largerin numerical value than the reduction rate; and an image cutting-outunit cutting out an image having the specified imaging FOV from theunfolded image.
 14. The magnetic resonance imaging system according toclaim 13, wherein the unfolding scale is an integer larger in numericalvalue than the reduction rate.
 15. A method of performing parallelimaging by a magnetic resonance imaging system provided with a multipleRF coil composed of a plurality of element coils and configured to usethe multiple RF coil to perform parallel imaging with an object to beimaged, said method comprising: specifying a desired imaging FOV (FieldOf View); specifying an acquisition FOV based on the imaging FOV, theacquisition FOV being used in performing a parallel imaging scan;specifying an unfolding FOV larger in size than the imaging FOV;performing the scan with the object based on the acquisition FOV so thata reconstructed image having the acquisition FOV is acquired for everyelement coil in response to the scan; applying, based on the unfoldingFOV, unfolding processing to the acquisition-FOV reconstructed image sothat the acquisition-FOV reconstructed image is unfolded to provide animage having the unfolding FOV; and producing an image having theimaging FOV from the unfolding-FOV image.